Open Access Article
Xuyang Luo,
Fei Gao
*,
Fengbiao Chen,
Qian Cheng,
Jinze Zhao,
Xiao Wei,
Cong Lin
,
Jiang Zhong
and
Liang Shen*
Jiangxi Engineering Laboratory of Waterborne Coating, School of Chemistry and Chemical Engineering, Jiangxi Science & Technology Normal University, Nanchang 330013, Jiangxi, P. R. China. E-mail: feigao2016@jxstnu.com.cn; liangshen@jxstnu.com.cn
First published on 21st April 2020
Novel organic–inorganic hybrid coating materials were developed using amino silanes and acetoacetylated soybean oil. The acetoacetylated soybean oil was prepared from soybean oil (a renewable resource) using a solvent-free method involving a thiol–ene and transesterification reactions, and the chemical structure was characterized by nuclear magnetic resonance (NMR), gel permeation chromatography (GPC), Fourier-transform infrared (FTIR) spectroscopy, and viscosity analyses. On the basis of the acetoacetylated soybean oil, several organic–inorganic hybrid coating materials were prepared using different amino silanes by a catalyst-free method involving one-step comprising two reactions (an amine–acetoacetate reaction and an in situ sol–gel technique), and their crosslinked structures were determined from their FT-IR and solid-state 29Si NMR spectra. The resulting coating materials have good mechanical/chemical performance. This method for preparing renewable organic–inorganic hybrid coating materials may have wide uses because plant oils contain many unsaturated C
C bonds and easy access to acetoacetate functional groups.
Acetoacetyl chemistry is interesting to use to prepare thermoset resins because acetoacetate functional groups can react with various groups,10–13 including aldehydes,14 isocyanates,15 acrylates,16 and amines.17 Although many thermoset resins have been prepared using acetoacetate chemistry and amines, only a few studies have been reported on the synthesis of biobased coating materials. Trumbo and co-workers18 developed novel biobased coating materials from multifunctional amines and acetoacetylated castor oil, and the properties of the coatings were found to be improved by increasing the temperature. Webster and co-workers19 invented novel biobased coating materials based on multifunctional amines and acetoacetylated sucrose, and the properties of the obtained coatings could be enhanced by adjusting the degree of substitution in the acetoacetylated sucrose. Recently, our group20 has reported biobased coating materials that were developed using modified acetoacetylated castor oil and multifunctional amines, and their properties were found to be improved upon increasing the acetoacetate group content. However, the preparation of organic–inorganic hybrid coating materials from acetoacetylated plant-based materials has not yet been reported.
Recently, we have been interested in the synthesis of organic–inorganic hybrid materials because of their novel chemical and physical properties.21,22 Silica-based hybrids are promising for use in the preparation of organic–inorganic hybrid materials, in which the condensation of organosiloxane precursors can be carried out a via sol–gel technique, and these materials are useful in many fields of technology, including electronic materials,23 separation science,24 solid electrolytes,25 as functional coatings,26 and so on.
In this work, we develop a novel organic–inorganic hybrid coating material based on acetoacetylated soybean oil, the reaction mechanism of which is shown in Scheme 1. The primary novelties of this study include: (1) acetoacetylated soybean oil is prepared from soybean oil via a solvent-free method, (2) organic–inorganic hybrids coating materials can be obtained in one step comprising two reactions (amine–acetoacetate reaction and in situ sol–gel technique), and (3) the method presented here is excellent for preparing renewable organic–inorganic hybrid coating materials because plant oils contain many unsaturated C
C bonds and provide easy access to acetoacetate functional groups.
![]() | ||
| Scheme 1 The reaction mechanism of the preparation of organic–inorganic hybrid coating materials via (a) an amine–acetoacetate reaction and (b) an in situ sol–gel technique. | ||
:
1 ratio based on the functional groups) and allowed to mix for 5 min. Then, water (1.5 mL) and ethanol (2 mL) were added to the system, which was mixed. The mixture was poured into a poly(tetrafluoroethylene) (PTFE) mold (8 × 8 × 1.5 cm), and finally, the films were cured via an amine–acetoacetate reaction and hydrolyzed in situ for 3 h at 30 °C, followed by 5 h at 80 °C, to give a dry film (350–450 micron thickness). In order to ensure full solvent removal, the films were further placed in a vacuum oven for 36 h at 60 °C.
| Sample code | Acetoacetylated soybean oil (mmol) | Cross-linker (mmol) | Acetoacetate/amine ratio |
|---|---|---|---|
| P1 | 0.591 | 2.96 (B1) | 1 : 1 |
| P2 | 0.591 | 2.96 (B2) | 1 : 1 |
| P3 | 0.591 | 2.96 (B3) | 1 : 1 |
1H and 13C NMR spectra were collected using a Bruker AV-400 NMR instrument, where tetramethylsilane (TMS) was used as an internal reference and deuterated chloroform (CDCl3) was used as a solvent. Solid-state 29Si NMR spectra were collected using a Fourier-transform Bruker 600 MHz wide bore solid spectrometer (model Avance III HD).
Thermogravimetric analysis (TGA) was performed using a TGA-Q50 system obtained from TA Instruments and the measurements were carried out from room temperature to 750 °C at a heating rate of 10 °C min−1 under a N2 atmosphere.
Dynamic mechanical analysis (DMA) of the films was performed using a (TA Instruments Q800, New Castle, De) dynamic mechanical analyzer with a film tension mode of 1 Hz. The samples were cooled in liquid nitrogen and held isothermally at −80 °C for 3 min, and then heated to 100 °C at a rate of 5 °C min−1. The storage moduli, loss moduli, and tan
δ of the films were studied under a controlled temperature.
The DSC experiments were performed on a TA calorimeter (TA-Q200, TA). The polymer sample was heated at a rate of 10 °C min−1 from −40–200 °C at a rate of 10 °C min−1 under a nitrogen atmosphere and heat capacity data of the samples were collected during the second heating process.
Gel permeation chromatography (GPC) was performed on a GPC apparatus (Waters 515; Waters, USA) at 25 °C. The samples were diluted to 2 mg mL−1 in THF for the GPC runs, where THF was used as an eluent at a flow rate of 1.0 mL min−1, and the molecular weights were determined using polystyrene standards.
A TA Discovery HR-2 Rheometer was used to measure the viscosity of the soybean oil (A1), modified soybean oil (A2), and modified acetoacetylated soybean oil (A3).
The gel content was determined by immersion of a film (2 × 2 cm piece) with a known weight (W1). The dried film was immersed in acetone for 48 h and then dehydrated for 48 h at 60 °C to provide a weight, W2. The gel content M (%) was then calculated according to the following formula: M (%) = W2/W1 × 100%.
C bonds per molecule, as confirmed by 1H NMR spectroscopy (Fig. S1a, ESI†). The chemical structure of the obtained acetoacetylated soybean oil was also confirmed by NMR, GPC, and FTIR spectroscopy. As shown in Fig. 1a, the peaks (soybean oil, A1) at 5.26 and 5.53 ppm ((c and d), correspond to the C
C bonds of the soybean oil) disappeared after the thiol–ene coupling reaction, and new peaks appeared at 3.68 and 3.85 ppm (e and f), which can be attributed to methyl carbons (grafting of 2-mercaptoethanol in the modified soybean oil (A2), by approximately 98%, Fig. S1b, ESI†). Compared to the acetoacetylated soybean oil (A3) and modified soybean oil (A2), the peaks at 3.68 and 3.85 ppm (e and f) shifted to 4.33–4.45 ppm (i) and the new peaks of the acetoacetyl group appeared at 3.5 ppm (g) and 2.36 ppm (h) (by approximately 93%, Fig. S2, ESI†). The 13C NMR spectra of the acetoacetylated soybean oil are shown in Fig. 1b. The intensities of the C
C bond peaks of the soybean oil (A1) at 126 ppm (B) and 130 ppm (C) decreased after the thiol–ene coupling reaction and new peaks for the acetoacetylated soybean oil (A3) appeared at 201 ppm (D) and 170 ppm (E). In addition, compared with the GPC curves of the soybean oil (A1), modified soybean oil (A2), and acetoacetylated soybean oil (A3) (Fig. S3, ESI†), the number average molecular weight was increased after the thiol–ene coupling reaction and transesterification reactions. These results show that acetoacetylated soybean oil was obtained.
The FTIR spectra of the acetoacetylated soybean oil are shown in Fig. 2. Comparing the spectrum of the soybean oil (A1) to that of the modified soybean oil (A2), new peak appears at 3430 cm−1 (D), corresponding to the absorption peak of the OH group, which indicates that the soybean oil reacted with 2-mercaptoethanol to gain OH groups. Comparing the modified soybean oil (A2) and acetoacetylated soybean oil (A3), the absorption band at 3430 cm−1 (D) in the acetoacetylated soybean oil (A3) disappeared and new peaks (acetoacetyl groups) appeared at 1740 cm−1 (B) and 1650 cm−1 (C). These results further confirmed that the acetoacetylated soybean oil was obtained.
![]() | ||
| Fig. 2 FTIR spectra of the soybean oil (A1), modified soybean oil (A2), and acetoacetylated soybean oil (A3). | ||
Fig. 3 shows the viscosities of soybean oil (A1), modified soybean oil (A2), and acetoacetylated soybean oil (A3). After the thiol–ene coupling reaction, the viscosity increased from 0.05 Pa s (soybean oil) to 6.5 Pa s (modified soybean oil) because of the increase in the number of intermolecular hydrogen bonds.27 However, after the transesterification reaction from modified soybean oil to acetoacetylated soybean oil, the viscosity decreased to 2.3 Pa s. The main reason for this was that the hydrogen bonding interactions were weakened by the transesterification reaction.
![]() | ||
| Fig. 3 Rheological viscosity versus the shear rate for soybean oil (A1), modified soybean oil (A2), and acetoacetylated soybean oil (A3). | ||
:
1 (for full experimental details see the Experimental section). The structures of the dried organic–inorganic hybrid coatings were determined by FTIR and solid-state 29Si NMR analyses. As shown in Fig. 4, the structures of the films (P1, P2, and P3), acetoacetylated soybean oil (A3), and crosslinkers (B1, B2, and B3) were confirmed from their FTIR spectra. The C
O stretching peaks (acetoacetylated soybean oil) at 1730 and 1650 cm−1 disappeared, and new peaks at 1640 cm−1 (C
O), 1605 cm−1 (C
C), and 3346 cm−1 (N–H) were observed in the three films. The absorption peaks at 1100 cm−1 (Si–O–Si asymmetric stretching), 1120 cm−1 (Si–O–Si symmetric stretching), 800 cm−1 (symmetrical Si–O–Si stretching), and 3400–3500 cm−1 (Si–OH groups) clearly demonstrate the success of using the sol–gel technique.28
![]() | ||
| Fig. 4 FTIR spectra of the three films (P1, P2, and P3), acetoacetylated soybean oil (A3), and the crosslinkers (B1, B2, and B3). | ||
The solid-state 29Si NMR of the three films (P1, P2, and P3) are shown in Fig. 5, which confirm the formation of the Si–O–Si bonds and network structure. In the spectra, only two peaks can be observed, and the peak at −68.46 ppm (T3 structure) is more obvious than the other peak (T2, −59.40 ppm), and the peak at −49.98 ppm (T1 structure) is almost absent.29 These results indicate that most of the network structure features one Si atom associated with three –Si–O–Si– linkages (T3), some of the network structure features one Si atom associated with two –Si–O–Si– linkages (T2), and a network structure with one Si atom associated with one –Si–O–Si– linkage (T1) is hardly observed. Due to the degree of branching (DB) being an important parameter used to describe the degree of similarity between the branched structure of hyperbranched polymers and ordinary dendritic polymers, it is usually determined from the integral area of the 29Si NMR spectrum according to Frey's equation: DB = 2D/(2D + L).30,31 Therefore, the DB values of the films were estimated to be 0.95, 0.93, and 0.88, all of which are close to 1, values that are obviously higher than those of traditional hyperbranched polymers. Thus, all three of the films may have a “completely branched” structure.32
| Sample code | Gel content (%) | Young's modulus (MPa) | Stress at break (MPa) | Elongation at break (%) | tan δ |
Tg (at tan δ) (°C) |
E′ at Tg + 50 °C (MPa) | Crosslink density (νe) (mol m−3) | TGA in nitrogen (°C) | DSC Tg (°C) | |||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| T5 | T10 | T50 | Tmax | ||||||||||
| a T5, T10, T50, and Tmax represent the temperatures at which the mass loss is 5, 10, and 50 wt%, and the maximum mass loss temperature, respectively. | |||||||||||||
| P1 | 98 | 486 ± 24 | 3.74 ± 0.51 | 1.16 ± 0.05 | 0.24 | 32 | 104 | 11 785 |
254 | 303 | 465 | 605 | 27 |
| P2 | 97 | 97 ± 5 | 2.89 ± 0.23 | 4.31 ± 0.24 | 0.32 | 28 | 87 | 9965 | 251 | 295 | 462 | 601 | 22 |
| P3 | 97 | 8 ± 0.5 | 0.43 ± 0.02 | 6.61 ± 0.41 | 0.57 | 22 | 41 | 4686 | 204 | 258 | 428 | 581 | 12 |
δ) dependent on the temperature for the three films (P1, P2, and P3) with different crosslinkers (B1, B2, and B3). The storage moduli (E′) of all of the films showed a similar trend with a change in temperature (Fig. 6a); with an increase in the temperature, the storage modulus (E′) decreased rapidly and finally stabilized. The loss factors (tan
δ) of these films are shown in Fig. 6b. Only one peak was observed in each case, indicating that the three films exhibit homogeneous properties. The glass transition temperature (Tg) was obtained according to the peak maximum value.
![]() | ||
Fig. 6 Dynamic mechanical analysis (DMA) of the three films (P1, P2, and P3): (a) storage modulus and (b) loss factor (tan δ) as a function of the temperature of the three films. | ||
The crosslink density was the calculated using the following formula:32–34
| νe = E′/3RT |
δ, and crosslinking density (νe) values of the three films are summarized in Table 2. Comparing the three films, P1 has the highest glass transition temperature (Tg) and crosslinking density. The main reason for this may be that the crosslinker C1 has a lower steric hindrance structure.
Fig. 7 presents the stress–strain curves of the films (P1, P2, and P3), and their tensile data (tensile strength, elongation at break, and Young's modulus) are shown in Table 2. Comparing the three films, it is obvious that P1 has the highest tensile strength and Young's modulus, but the lowest elongation at break value, and P3 has the lowest tensile strength and Young's modulus, but the highest elongation at break value, which may be because as the crosslinking density decreases, the mechanical properties (tensile strength and Young's modulus) gradually decrease.35
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/d0ra01279c |
| This journal is © The Royal Society of Chemistry 2020 |